• Title/Summary/Keyword: B&O

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Superexchange Interactions in Spinel Ferrites (Spinel Ferrite에서의 초교환 상호작용)

  • 이충섭;이찬영
    • Journal of the Korean Magnetics Society
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    • v.3 no.3
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    • pp.173-178
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    • 1993
  • We have calculated the reduced spontaneous magnetization in different environments and average value as func¬tion of reduced temperature of the magnetic ions(Fe) for A(tetrahedral) and B(octahedral) sites in spinel ferrites $AB_{2}O_{4}$ using A-O-B superexchange interaction. The reduced spontaneous magnetization and average value by A-O-B superexchange interaction are compared with that by A-B direct interaction. To contrast A-O-B superexchange interaction with A-B direct interaction, $M\"{o}ssbauer$ spectra from previous two interactions are obtained.

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Electrical and Optical properties of B-doped ZnO films Deposited by RF Magnetron Sputtiering (RF 마그네트론 스퍼터링법으로 증착한 B-doped ZnO 박막의 전기 및 광학적 특징)

  • 임주수;이재신
    • Journal of the Korean Ceramic Society
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    • v.35 no.1
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    • pp.17-22
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    • 1998
  • B-doped ZnO thin films on glass substrates were prepared by sputtering the ceramic targets which had been prepared by sintering disks consisting of ZnO and various amounts of B2O3 While pure ZnO films show-ed a c-axis oriented growth the B-doping retarded the prefered orientation and grain growth of the film. Electron concentrations for undoped and B-doped ZnO films were on the order of 7.8${\times}$1018 cm-3 and 5${\times}${{{{ {10 }^{20 } }} c{{{{ {m }^{-3 } }} respectively. The electron mobility however decreased with the B-doping concentration. Optical meas-urements on the films showed that the average transmittance in the visible range was higher than 85% The measurements also indicated a blueshift of the absorption edge with doping.

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Phase Separation and their Structures in $BaO-B_2O_3$ Glasses ($BaO-B_2O_3$계 유리의 상분리 현상과 유리의 구조)

  • 채수철;김철영
    • Journal of the Korean Ceramic Society
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    • v.23 no.6
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    • pp.25-32
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    • 1986
  • Phase spearated glass is heterogeneous in microscopic point of view and the heterogeneities affect the structures of glasses. In the present work the phase separation of $BaO-B_2O_3$ glass system was investigated and the effect of $P_2O_5$ on the phase separation and crystallization was also studied in the above system. Experiments such as scanning electron microscopy X-ray diffraction and infrared spectroscopy were performed. Phase separation with $B_2O_3$ rich phase matrix and BaO rich phase droplet was observed for the glasses containing less than 6 mole% of BaO while the opposite morphology of phase separation was found for the glasses containing more than 7 mole% of BaO. Phase separation region was extended up to the glass with 22mole% of BaO when the amount of $P_2O_5$ was increased. The heat-treated glasses crystallized to BaO.$4B_2O_3$$P_2O_5$ hindered the glass from the crystalli-zation.

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Effect of B2O3 Additives on GaN Powder Synthesis from GaOOH (GaOOH로부터 GaN 분말의 합성에 미치는 B2O3의 첨가효과)

  • Song, Changho;Shin, Dongwhee;Byun, Changsob;Kim, Seontai
    • Korean Journal of Materials Research
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    • v.23 no.2
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    • pp.104-111
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    • 2013
  • In this study, GaN powders were synthesized from gallium oxide-hydroxide (GaOOH) through an ammonification process in an $NH_3$ flow with the variation of $B_2O_3$ additives within a temperature range of $300-1050^{\circ}C$. The additive effect of $B_2O_3$ on the hexagonal phase GaN powder synthesis route was examined by X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS) and Fourier transformation infrared transmission (FTIR) spectroscopy. With increasing the mol% of $B_2O_3$ additive in the GaOOH precursor powder, the transition temperature and the activation energy for GaN powder formation increased while the GaN synthesis limit-time ($t_c$) shortened. The XPS results showed that Boron compounds of $B_2O_3$ and BN coexisted in the synthesized GaN powders. From the FTIR spectra, we were able to confirm that the GaN powder consisted of an amorphous or cubic phase $B_2O_3$ due to bond formation between B and O and the amorphous phase BN due to B-N bonds. The GaN powder synthesized from GaOOH and $B_2O_3$ mixed powder by an ammonification route through ${\beta}-Ga_2O_3$ intermediate state. During the ammonification process, boron compounds of $B_2O_3$ and BN coated ${\beta}-Ga_2O_3$ and GaN particles limited further nitridation processes.

Ferroelectric Properties of Ti-Doped and W-Doped SBT Ceramics (Ti와 W이 첨가된 SBT 세라믹스의 강유전 특성)

  • 천채일;김정석
    • Journal of the Korean Ceramic Society
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    • v.41 no.5
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    • pp.401-405
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    • 2004
  • Undoped SrB $i_2$T $a_2$O$_{9}$, donor-doped Sr$_{0.99}$B $i_2$(Ta$_{0.99}$W$_{0.01}$)$_2$O$_{9}$ and acceptor-doped SrB $i_2$(Ta$_{0.99}$Ti$_{0.01}$)$_2$O$_{8.99$ ceramics were prepared and their microstructure, ferroelectric P-E hysteresis and Curie temperature were investigated. Grain size did not influence P-E hysteresis curve in undoped SrB $i_2$T $a_2$O$_{9}$ ceramics. Donor-Doped Sr$_{0.99}$B $i_2$(Ta$_{0.99}$W$_{0.01}$)$_2$O$_{9}$ ceramics showed more saturated P-E hysteresis curve with larger remanent polarization (P$_{r}$) than undoped SrB $i_2$T $a_2$O$_{9}$ ceramics while acceptor-doped SrB $i_2$(Ta$_{0.99}$Ti$_{0.01}$)$_2$O$_{8.99}$ ceramics led to a pinched P-E hysteresis loop. Larger polarization in donor-doped Sr$_{0.99}$B $i_2$(Ta$_{0.99}$W$_{0.01}$)$_2$O$_{9}$ ceramics resulted from easier domain wall motion by Sr-vacancies.

Control of carrier concentrations by addition of $B_{2}O_{3}$ in Si-doped vertical gradient freeze (VGF) GaAs single crystal growth (수직경사응고(VGF)법에 의한 Si 도핑 GaAs 단결정 성장시 $B_{2}O_{3}$ 첨가에 따른 캐리어 농도 변화)

  • Bae, So-Ik;Han, Chang-Woon
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.19 no.2
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    • pp.75-78
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    • 2009
  • Si-doped GaAs single crystals were grown by vertical gradient freeze using PBN crucibles. The amount of oxide layer $B_{2}O_{3}$ in PBN crucible was changed($0{\sim}0.2wt%$) and measured the concentration of carriers. The segregation coefficients of Si in GaAs melt decreased rapidly from initial 0.1 to 0.01 as the amount of $B_{2}O_{3}$ increases. At the same time, concentration of carriers was shown to decrease. It is likely that the reaction between dopant Si and $B_{2}O_{3}$ in GaAs melt results in the reduction of Si dopants(donor) while increase in the amount of boron(acceptor). The thin layer of $B_{2}O_{3}$ glass in PBN crucible was proved to be a better way to reduce defect formation rather than the total amount of $B_{2}O_{3}$.

pH Dependence on the Degradation of Rhodamine B by Fe-ACF/$TiO_2$ Composites and Effect of Different Fe Precursors (Fe-ACF/$TiO_2$ 복합체에 의한 로다민 B 용액의 분해에 있어서 pH 의존성 및 여러 가지 Fe 전구체의 효과)

  • Zhang, Kan;Oh, Won-Chun
    • Elastomers and Composites
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    • v.44 no.4
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    • pp.408-415
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    • 2009
  • Iron-loaded activated carbon fibers (Fe-ACF) supported titanium dioxide ($TiO_2$) photocatalyst (Fe-ACF/$TiO_2$) was synthesized using a sol-gel method. Three different types of Fe-ACF/$TiO_2$ were obtained by treatment with different precursor of Fe, and characterized using BET, SEM, XRD and EDX analysis. The photocatalytic activity of Fe-ACF/$TiO_2$ was investigated by the degradation of Rhodamine B (Rh.B) solution under UV irradiation. From the experimental results, it was revealed that Fe-ACF/$TiO_2$ composites show considerable photocatalytic ability for the removal of Rh.B by comparing non-treated ACF/$TiO_2$ composites. And photo-Fenton reaction with Fe element was incoordinately influenced due to different precursor of Fe. It clearly indicates that Fe-ACF/$TiO_2$ composites prepared using $FeCl_3$ provided the highest photo-Fenton activity, then, which was affected by pH changes on the degradation of Rh.B.

Study on Low-Temperature sintering of Co2Z type Ba ferrites for chip inductor (Chip inductor용 Co2Z type Ba-ferrite의 저온소결에 관한 연구)

  • 조균우;한영호;문병철
    • Journal of the Korean Magnetics Society
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    • v.12 no.5
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    • pp.195-200
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    • 2002
  • Low temperature sintering of Co$_2$Z type Ba ferrites with various oxide additives has been studied. Co$_2$Z phase was obtained by 2 step calcination and XRD peaks showed a good agreement with the peaks of the standard Co$_2$Z phase, except for some minor extra peaks. ZnO-B$_2$O$_3$ glass, ZnO-B$_2$O$_3$ and CuO, ZnO-B$_2$O$_3$ and Bi$_2$O$_3$, and ZnO-Bi$_2$O$_3$ glass were added to lower sintering temperatures. Specimens were sintered at the temperature range between 900 $^{\circ}C$ and 1000 $^{\circ}C$. In the single addition of ZnO-B$_2$O$_3$ glass, the specimen with 7.5 wt% showed the highest shrinkage. Specimens with complex addition of ZnO-B$_2$O$_3$ glass with CuO or Bi$_2$O$_3$ showed higher shrinkages and initial permeabilities than single addition of ZnO-B$_2$O$_3$ glass. Shrinkages and initial permeabilities of the specimens with ZnO-Bi$_2$O$_3$ glass were higher than those of ZnO-B$_2$O$_3$ glass addition.

Dielectric/piezoelectric Properties of Mn-Doped PMN-PZT with Variations of the Sintering Temperature and Addition of B2O3 (소결온도와 B2O3첨가량에 따른 Mn첨가 PMN-PZT의 유전 및 압전특성의 변화)

  • Shin Hyo-Soon
    • Journal of the Korean Ceramic Society
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    • v.41 no.9
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    • pp.709-714
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    • 2004
  • The additive of low temperature sintering in Mn-doped PMN-PZT known as high piezoelectric materials was studied in this experiment. B$_2$O$_3$ was used for the additive of low temperature sintering. The effects of sintering temperature in dielectric, and piezoelectric properties were investigated with the amounts of B$_2$O$_3$. Sintered density was increased in comparison with no addition and under 2wt% B$_2$O$_3$ and lower sintering temperature than 100$0^{\circ}C$. Therefore, in the low sintering temperature, the densification was improved by the addition of the B$_2$O$_3$. However, the sintering density was lower than that of the main composition in the case of the sintered at over 10$50^{\circ}C$. Dielectric constant with the addition of B$_2$O$_3$ was evaluated. The dielectric constant was 1000 2 wt% of B$_2$O$_3$ and sintered at 100$0^{\circ}C$. Under 2wt% of B$_2$O$_3$, the electromechanical coupling factor and the piezoelectric constant were not so much decreased. The electromechanical coupling factor and the piezoelectric constant were 50% and 300(${\times}$10$^{-12}$ C/N) respectively. The mechanical quality factor was increased with B$_2$O$_3$. The mechanical quality factor was 1700 at 0.5wt% B$_2$O$_3$ and sintered at 110$0^{\circ}C$. Dielectric loss was less than 0.5% regardless of the amount of B$_2$O$_3$.